Journal of Applied Mathematics and Physics
Vol.03 No.07(2015), Article ID:57573,4 pages
10.4236/jamp.2015.37088
On No-Node Solutions of the Lazer-McKenna Suspension Bridge Models
Fanglei Wang, Kangbao Zhou
College of Science, Hohai University, Nanjing, China
Received 3 March 2015; accepted 23 June 2015; published 30 June 2015
ABSTRACT
In this paper, we are concerned with the existence and multiplicity of no-node solutions of the Lazer-McKenna suspension bridge models by using the fixed point theorem in a cone.
Keywords:
Differential Equations, Periodic Solution, Cone, Fixed Point Theorem
1. Introduction
In [1], the Lazer-McKenna suspension bridge models are proposed as following
If we look for no-node solutions of the form and impose a forcing term of the form, then via some computation, we can obtain the following system:
(1)
In this paper, by combining the analysis of the sign of Green's functions for the linear damped equation, together with a famous fixed point theorem, we will obtain some existence results for (1) if the nonlinearities satisfy the following semipositone condition
(H) The function is bounded below, and maybe change sign, namely, there exists a sufficiently large constant M > 0 such that
Such case is called as semipositone problems, see [2]. And one of the common techniques is the Krasnoselskii fixed point theorem on compression and expansion of cones.
Lemma 1.1 [3]. Let be a Banach space,and be a cone in. Assume, are open subsets of with, , Let be a completely continuous operator such that either
(i); or
(ii);
Then, has a fixed point in
2. Preliminaries
If the linear damped equation
(2)
is nonresonant, namely, its unique T-periodic solution is the trivial one, then as a consequence of Fredholm’s alternative in [4], the nonhomogeneous equation admits a unique T-periodic solution
which can be written as where G(t; s) is the Green’s function of (2). For convenience,
we will assume that the following standing hypothesis is satisfied throughout this paper:
(H1) are T-periodic functions such that the Green’s function, associated with the linear damped equation
is positive for all, and
(H2) are negative T-periodic functions, and satisfy:
Let E denote the Banach space with the norm for. Define K to a cone in E by where. Also, for r > 0 a positive number, let
If (H), (H1) and (H2) hold, let, (1) is transformed into
(3)
where is chosen such that
Let be a map, which defined by, where
t is straightforward to verify that the solution of (1) is equivalent to the fixed point Equation
Lemma 2.1 Assume that (H), (H1) and (H2) hold. Then is compact and continuous.
For convenience, define, for any.
Lemma 2.2 [2] Assume that (H), (H1) and (H2) hold. If, then, for i = 1, 2, the functions are continuous on, for, and
Lemma 2.3 [2] Assume that (H), (H1) and (H2) hold. If, then, for i = 1, 2, the functions are continuous on, for, and
3. Main Results
Theorem 3.1 Assume that (H), (H1) and (H2) hold.
(I) Then there exists a such that (1) has a positive periodic solution for
(II) If, then for an, (1) has a positive periodic solution;
(III) If, then (1) has two positive periodic solutions for all sufficiently small.
Proof. (I) On one hand, take R > 0 such that
Set Then, for each, we have
Then from the above inequalities, it follows that there exists a such that
Furthermore, for any, we obtain
In the similar way, there exists a, such that and we also have
So let us choose and we can obtain
On the other hand, from the condition for all, it follows that there is a sufficient small r > 0 such that for and where is chosen such that
Then, for any, we obtain
So we have
Therefore, from Lemma 1.1, it follows that the operator B has at least one fixed point in, for
(II) Since, then from Lemma 2.1, it follows that Define a function as By Lemma 2.5 in [2], it is easy to see that Thus by the definition, there is an such that where satisfying
Then, for each, we have
In the similar way, for any, we also have Furthermore, from The above inequalities, we get
Therefore, from Lemma 1.1, it follows that B has one fixed point in for any
(III) Since, then from Lemma 2.2, it follows that By the definition, there exists such that where is chosen such that
Choosing and for any, we have and
Thus from the above inequalities, we can get
Therefore, from Lemma 1.1, it follows that the operator B has at least two fixed points in and in. Namely, system (1) has two solutions for sufficiently small
Cite this paper
Fanglei Wang,Kangbao Zhou, (2015) On No-Node Solutions of the Lazer-McKenna Suspension Bridge Models. Journal of Applied Mathematics and Physics,03,737-740. doi: 10.4236/jamp.2015.37088
References
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